Rescic J, Vlachy V, Bhuiyan L B, Outhwaite C W
Faculty of Chemistry and Chemical Technology, University of Ljubljana, 1000 Ljubljana, Slovenia.
Langmuir. 2005 Jan 4;21(1):481-6. doi: 10.1021/la049285+.
The catalytic effect of charged micelles as manifested through the increased collision frequency between the counterions of an electrolyte in the presence of such micelles is explored by the Monte Carlo simulation technique and various theoretical approaches. The micelles and ions are pictured as charged hard spheres embedded in a dielectric continuum with the properties of water at 298 K with the charge on micelles varying from zero to z(m) = 50 negative elementary charges. Analytical theories such as (i) the symmetric Poisson-Boltzmann theory, (ii) the modified Poisson-Boltzmann theory, and (iii) the hypernetted-chain integral equation are applied and tested against the Monte Carlo data for micellar ions (m) with up to 50 negative charges in aqueous solution with monovalent counterions (c; z(c) = +1) and co-ions (co; z(co) = -1). The results for the counterion-counterion pair correlation function at contact, g(cc)(sigma(cc)), are calculated in a micellar concentration range from c(m) = 5 x 10(-)(6) to 0.1 mol/dm(3) with an added +1:-1 electrolyte concentration of 0.005 mol/dm(3) (for most cases), and for various model parameters. Our computations indicate that even a small concentration of a highly charged polyelectrolyte added to a +1:-1 electrolyte solution strongly increases the probability of finding two counterions in contact. This result is in agreement with experimental data. For low charge on the micelles (z(m) below -8), all the theories are in qualitative agreement with the new computer simulations. For highly charged micelles, the theories either fail to converge (the hypernetted-chain theory) or, alternatively, yield poor agreement with computer data (the symmetric Poisson-Boltzmann and modified Poisson-Boltzmann theories). The nonlinear Poisson-Boltzmann cell model results yield reasonably good agreement with computer simulations for this system.
通过蒙特卡罗模拟技术和各种理论方法,研究了带电胶束在电解质反离子存在下,通过增加碰撞频率所表现出的催化作用。胶束和离子被视为嵌入具有298K水性质的介电连续介质中的带电硬球,胶束上的电荷从零变化到(z_m = 50)个负基本电荷。应用了诸如(i)对称泊松 - 玻尔兹曼理论、(ii)修正泊松 - 玻尔兹曼理论和(iii)超网链积分方程等分析理论,并针对含有单价反离子((c);(z_c = +1))和共离子((co);(z_{co} = -1))的水溶液中带有多达50个负电荷的胶束离子((m))的蒙特卡罗数据进行了测试。在胶束浓度范围从(c_m = 5×10^{-6})到(0.1) (mol/dm^3),添加的(+1:-1)电解质浓度为(0.005) (mol/dm^3)(大多数情况)以及各种模型参数下,计算了接触时反离子 - 反离子对关联函数(g_{cc}(\sigma_{cc}))的结果。我们的计算表明,即使向(+1:-1)电解质溶液中添加少量高电荷聚电解质,也会大大增加发现两个反离子接触的概率。这一结果与实验数据一致。对于胶束上低电荷((z_m)低于 -8)的情况,所有理论与新的计算机模拟在定性上一致。对于高电荷胶束,理论要么无法收敛(超网链理论),要么与计算机数据的一致性较差(对称泊松 - 玻尔兹曼理论和修正泊松 - 玻尔兹曼理论)。非线性泊松 - 玻尔兹曼元胞模型结果与该系统的计算机模拟结果相当吻合。